TECHNICAL FIELD
[0001] This disclosure relates generally to computer systems, and specifically to a clock
distribution system.
BACKGROUND
[0002] Typical circuits that implement logic functions can operate based on a clock to synchronize
data and/or provide a time-based flow of the logic functions. Circuits that are based
on complementary metal-oxide-semiconductor (CMOS) technology can implement a clock
to indicate when a given logic circuit or gate is to capture data at one or more inputs
for processing or transferring the data to other logic functions. A given clock can
thus provide a clock signal to a variety of devices in the circuit to provide the
requisite timing information, and thus to substantially synchronize data transfer
and timing functions. Other types of circuits can implement clock signals, such as
reciprocal quantum logic (RQL) circuits. RQL circuits can implement timing information
based on a clock that is provided, for example, as a sinusoidal signal having a substantially
stable-frequency.
SUMMARY
[0003] One example includes a clock distribution system. The system includes a resonator
feed network comprising a plurality of resonant transmission lines that each propagate
a clock signal. The system also includes at least one resonator spine. Each of the
at least one resonator spine can be conductively coupled to at least one of the resonant
transmission lines, such that each of the at least one resonator spine propagates
the clock signal. The system further includes at least one resonator rib conductively
coupled to at least one of the at least one resonator spine. Each of the at least
one resonator rib can be arranged as a standing wave resonator to propagate the clock
signal.
[0004] Another example includes a clock distribution system. The system includes a resonator
feed network comprising a plurality of resonant transmission lines that each propagate
a clock signal. The system also includes at least one resonator spine. Each of the
at least one resonator spine can be conductively coupled to at least one of the resonant
transmission lines a plurality of the resonant transmission lines of the resonator
feed network at each of a plurality of locations separated by at least one interval
along a length of the respective one of the at least one resonator spine, such that
each of the at least one resonator spine propagates the clock signal. The system further
includes at least one resonator rib conductively coupled to at least one of the at
least one resonator spine. Each of the at least one resonator rib can be arranged
as a standing wave resonator to propagate the clock signal.
[0005] Another example includes a clock distribution system. The system includes a resonator
feed network comprising a first set of resonant transmission lines and a second set
of resonant transmission lines. Each of the first and second sets of resonant transmission
lines can have a quantity greater than one and can be configured to propagate a clock
signal. The system also includes a first resonator spine conductively coupled to the
first set of resonant transmission lines, such that the first resonator spine propagates
the clock signal, and a second resonator spine conductively coupled to the second
set of resonant transmission lines, such that the second resonator spine propagates
the clock signal. The system further includes at least one resonator rib conductively
coupled to each of the first and second resonator spines. Each of the at least one
resonator rib can be arranged as a standing wave resonator to propagate the clock
signal.
BRIEF DESCRIPTION OF THE DRAWINGS
[0006]
FIG. 1 illustrates an example of a clock distribution system.
FIG. 2 illustrates an example of a resonator feed network.
FIG. 3 illustrates another example of a clock distribution system.
FIG. 4 illustrates another example of a clock distribution system.
FIG. 5 illustrates an example diagram of resonator spines.
FIG. 6 illustrates another example diagram of resonator spines.
FIG. 7 illustrates another example diagram of resonator spines.
FIG. 8 illustrates an example of a resonator feed network.
FIG. 9 illustrates another example of a clock distribution system.
DETAILED DESCRIPTION
[0007] This disclosure relates generally to computer systems, and specifically to a clock
distribution system. The clock distribution system, as described herein, is arranged
as a resonator "spine" and "rib" configuration. As described herein, the term "spine",
as pertaining to the resonator, describes a conductor that is configured to propagate
a clock signal (e.g., an in-phase or quadrature-phase clock signal). The term "rib",
as pertaining to the resonator, describes a conductor that is conductively coupled
to the spine and is arranged as a standing-wave resonator that propagates the clock
signal. The clock distribution system can include a plurality of resonator ribs that
are each conductively coupled to the same resonator spine, and thus can each separately
propagate the clock signal from the resonator spine. For example, the clock distribution
system can be arranged as dynamic zeroth-order resonators ("DynaZORs") that implement
a resonator "spine" and "rib" configuration, such as described in
U.S. Patent No. 10,133,299 (Attorney Docket No. NG(ES)-027022 US PRI), which is incorporated herein by reference
in its entirety.
[0008] The clock distribution system includes a resonator feed network that includes a plurality
of resonant transmission lines that are each configured to propagate a clock signal
(e.g., a sinusoidal clock signal). As an example, each of the resonant transmission
lines of the resonator feed network are conductively coupled to each other and to
a clock source at a first end of each of the resonant transmission lines. For example,
each of the resonant transmission lines can include at least one transmission line
having a predetermined length, such that each of the resonant transmission lines can
have a total length of approximately one-half of a wavelength of the clock signal.
[0009] The clock distribution system also includes at least one resonator spine that is
conductively coupled to at least one of the resonant transmission lines of the resonator
feed network. Therefore, the resonator spine(s) can likewise propagate the clock signal.
For example, the clock distribution system can include a plurality of resonator spines
that are each conductively coupled to at least one of the resonant transmission lines.
Each of the resonator spines can therefore be coupled to multiple resonant transmission
lines (e.g., at predefined intervals along the length of the resonator spine(s). Because
each of the resonant transmission lines can be coupled together at a first end and
have approximately one-half wavelength total length, the distance between any two
given conductive couplings of respective resonant transmission lines to the resonator
spine(s) can have a total length of approximately one wavelength, and therefore approximately
equal amplitude. As a result, the coupling of the resonator(s) to the resonator spine(s)
can increase uniformity of amplitude of the clock signal along the length of the resonator
spine(s). Furthermore, amplitude aberrations of other frequency modes of the clock
signal can be suppressed to provide for further uniformity of the amplitude of the
clock signal. Accordingly, amplitude variations of the clock signal resulting from
frequency mode deviations based on fabrication process variations of a given integrated
circuit (IC) can be mitigated.
[0010] FIG. 1 illustrates an example of a clock distribution system 100. The clock distribution
system 100 can be implemented in a variety of applications, such as superconducting
circuits (e.g., a reciprocal quantum logic (RQL) circuits). For example, the clock
distribution system 10 can be implemented in or as part of an integrated circuit (IC).
[0011] The clock distribution system 100 includes at least one resonator system 102. As
described herein, the term "resonator system" describes at least one resonator that
includes a spine and rib architecture to propagate a clock signal CLK. As an example,
the clock signal CLK can be a sinusoidal clock signal. The resonator system(s) 102
can be configured to provide the clock signal CLK (e.g., generated from an oscillator)
to each of a respective one or more circuits 104 that may be distributed across an
IC in which the clock distribution system 100 is implemented, as described herein.
In the example of FIG. 1, each of the resonator system(s) 102 includes at least one
resonator feed network 106, at least one resonator spine 108, and at least one resonator
rib 110. The resonator spine(s) 108 are conductively coupled to at least one resonator
of the resonator feed network(s) 106, and the resonator rib(s) 110 are each conductively
coupled to a given one or more of the resonator spine(s) 108. Thus, the clock signal
CLK, provided to the resonator feed network(s) 106 (e.g., from a local oscillator),
can be provided to propagate through the resonator feed network(s), through the resonator
spine(s) 108, and through each of the respective resonator rib(s) 110.
[0012] In the example of FIG. 1, the circuit(s) 104 are coupled to the resonator rib(s)
110, such as inductively via respective transformer-coupling lines, to provide a clock
current I
CLK to an associated one of the circuit(s) 104. Therefore, the clock current I
CLK can be provided to the circuit(s) 104 to provide functions (e.g., timing functions
and/or power distribution functions) for the associated circuit(s) 104. Because the
circuit(s) 104 can be distributed across the respective IC, substantial uniformity
of the clock signal CLK can provide for more accurate timing and interaction between
the circuit(s) 104. Furthermore, due to fabrication and process tolerance mismatches,
the frequency of the clock signal CLK can vary relative to the resonant frequency
of the resonant transmission lines that form the resonator feed network(s) 106, the
resonator spine(s) 108, and the resonator rib(s) 110. The frequency variations of
the clock signal CLK can provide for off-resonance frequency modes of the clock signal
CLK on a given IC or between separate ICs, which can vary the amplitude of the clock
signal CLK along a given length of the resonator spine(s) 108. To mitigate variations
in amplitude along the length of the resonator spine(s) 108, as described herein,
there can be a multitude of different configurations of the connection of the resonant
transmission lines of the resonator feed network(s) 106 to the respective resonator
spine(s) 108.
[0013] FIG. 2 illustrates an example of a resonator feed network 200. As an example, the
resonator feed network 200 can be coupled to a carrier supporting one or more ICs
(e.g., via bump bonds) to provide the clock signal CLK to the remaining portions of
a given resonator system (e.g., resonator spine(s)), as described herein. The resonator
feed network 200 can correspond to one of the resonator feed network(s) 106 in the
example of FIG. 1. Therefore, reference is to be made to the example of FIG. 1 in
the following description of the example of FIG. 2.
[0014] The resonator feed network 200 includes an oscillator 202 configured to generate
a clock signal CLK. As an example, the clock signal CLK can be a sinusoidal clock
signal, and can correspond to one of the components of a quadrature RQL clock signal
(e.g., an in-phase component or a quadrature-phase component). In the example of FIG.
2, the resonator feed network 200 also includes a plurality of resonant transmission
lines 204. The resonant transmission lines 204 are demonstrated as conductively coupled
together and to the oscillator 202 at a node 206 at a first end, and include respective
outputs 208 at a second end. In the example of FIG. 2, the outputs 208 are demonstrated
as a quantity of eleven, and thus provide respective approximately identical clock
signals CLK
A through CLK
K. However, other quantities greater than or less than eleven are possible for the
clock distribution system, as described herein. As described herein, the clock signals
CLK
A through CLK
K correspond to approximately equal copies of the clock signal CLK, and are therefore
all approximately equal with respect to frequency and amplitude.
[0015] In the example of FIG. 2, the resonant transmission lines 204 are each demonstrated
as including two transmission line segments 210. Each of the transmission line segments
210 is demonstrated as having a length of "λ/4", and thus one-quarter of the wavelength
"λ" of the clock signal CLK. However, the lengths of the transmission line segments
210 can deviate from one quarter wavelength, and are hereinafter understood to be
approximately λ/4. Therefore, the total length of each of the resonant transmission
lines 204 is approximately λ/2, and thus approximately half the wavelength of the
clock signal CLK. As a result, the length between any two of the outputs 208, through
a total of four of the transmission line segments 210, is approximately one wavelength
"λ" of the clock signal CLK. Therefore, the amplitude of the clock signal CLK at each
of the outputs 208 is approximately equal. As described herein, the example of FIG.
2 is demonstrated diagrammatically, such that the distance between resonant transmission
lines 204 at the node 206 is negligible (e.g., approximately zero).
[0016] As described in greater detail herein, the outputs 208 of the resonant transmission
lines 204 are coupled to the resonator spine(s) of the clock distribution system.
For example, the resonant transmission lines 204 can include two separate λ/4 length
transmission line segments 210, as demonstrated in the example of FIG. 2, to improve
frequency and amplitude response of the resonator 204. As an example, there can be
an impedance mismatch between the transmission line segment 210 that is coupled to
resonator spine at the respective output 208 and the transmission line segment 210
coupled to the oscillator 202 (and the other resonant transmission lines 204). However,
the resonant transmission lines 204 can instead include transmission line segments
of other lengths, such as a single λ/2 length transmission line segment, or any other
even multiple of λ/4 length transmission line segments.
[0017] FIG. 3 illustrates another example of a clock distribution system 300. The clock
distribution system 300 can correspond to a portion of the clock distribution system
102 in the example of FIG. 1. Therefore, reference is to be made to the example of
FIGS. 1 and 2 in the following description of the example of FIG. 3.
[0018] The clock distribution system 300 includes a plurality K of resonator spines 302,
where K corresponds to the eleventh one of the resonator spines 302. The clock distribution
system 300 also includes a plurality of sets of resonator ribs 304 that are coupled
to each of the resonator spines 302. As described above, the clock distribution system
300 can include circuits (not shown in the example of FIG. 3) that are coupled (e.g.,
inductively) to the resonator ribs 304. In the example of FIG. 3, each of the resonator
spines 302 receives the clock signal CLK, demonstrated as the respective clock signals
CLK
A through CLK
K as described above. Therefore, each of the resonator spines 302 is coupled to one
of the outputs 208 of the respective resonant transmission lines 204 in the example
of FIG. 2.
[0019] In the example of FIG. 3, the clock signals CLK
A through CLK
K are provided at approximately a midpoint along the length of the resonator spines
302. As an example, the resonator spines 302 can all be approximately the same length,
which can be approximately equal to a wavelength λ or a multiple of the wavelength
of the clock signal CLK. As a result, the resonator spines 302 can operate as standing-wave
resonators. For example, the resonator ribs 304 can be conductively coupled to the
respective resonator spines 302 at approximate antinode portions of the respective
clock signals CLK
A through CLK
K propagating in standing-wave manner on the respective resonator spines 302. Therefore,
the resonator ribs 304 can each propagate the respective one of the clock signals
CLKA through CLK
K at an approximately equal amplitude to provide uniformity of the clock current I
CLK to respective circuits that are coupled to the resonator ribs 304.
[0020] Additionally, because each of the resonator spines 302 is provided a respective one
of the clock signals CLK
A through CLK
K, the resonator spines 302 can propagate the clock signal CLK approximately uniformly
with respect to each other, as opposed to typical resonator systems that provide a
clock signal to one resonator (e.g., resonator spine) of a group of resonator spines
that implement conductive cross-connections between them (e.g., through ribs or other
conductors between the respective resonator spines 302). For example, as described
above, the length from one of the resonator spines 302 to any other one of the resonator
spines 302 through the resonant transmission lines 204 that provide the respective
clock signals CLK
A through CLK
K is approximately one wavelength λ of the clock signal CLK. Therefore, the resonator
spines 302 are all conductively coupled through the resonant transmission lines 204,
and the amplitude of the clock signals CLK
A through CLK
K can be approximately uniformly applied to each of the resonator spines 302. As a
result, the clock distribution system 300 can exhibit greater uniformity of the clock
signal CLK in each of the resonator spines 302 relative to an arrangement in which
the clock signal CLK is provided to only one of the resonator spines 302 that are
conductively coupled through cross-bars or the resonator ribs 304.
[0021] FIG. 4 illustrates another example of a clock distribution system 400. The clock
distribution system 400 can correspond to a portion of the clock distribution system
102 in the example of FIG. 1. Therefore, reference is to be made to the example of
FIGS. 1 and 2 in the following description of the example of FIG. 4.
[0022] The clock distribution system 400 includes a first resonator spine 402 and a second
resonator spine 404. The clock distribution system 400 also includes a plurality of
sets of resonator ribs 408 that are coupled to each of the resonator spines 402 and
404. As an example, the first and second resonator spines 402 and 404 can nominally
be fabricated to be approximately equal in length. As a first example, each of the
resonator ribs 408 can be coupled to the resonator spines 402 and/or 404. As described
above, the clock distribution system 400 can include circuits (not shown in the example
of FIG. 4) that are coupled (e.g., inductively) to the resonator ribs 408.
[0023] The resonator spines 402 and 404 receive the clock signal CLK, demonstrated as the
respective clock signals CLK
A through CLK
K as described above. In the example of FIG. 4, the clock signals CLK
A through CLK
F are provided to the first resonator spine 402 and the clock signals CLK
G through CLK
K are provided to the second resonator spine 404. The clock signals CLK
A through CLK
K can be provided at locations along the length of the resonator spines 402 and 404
at predetermined equal intervals between the sets of resonator ribs 408. As an example,
the intervals between each of the conductive coupling of the clock signals CLKA through
CLK
F to the first resonator spine 402 and the intervals between each of the conductive
coupling of the clock signals CLK
G through CLK
K to the second resonator spine 404 can be approximately equal along the length of
the respective first and second resonator spines 402 and 404.
[0024] Based on the coupling of multiple copies of the clock signal CLK (e.g., the clock
signals CLK
A through CLK
F to the first resonator spine 402 and the clock signals CLK
G through CLK
K to the second resonator spine 404), the clock signal CLK can propagate on the first
and second resonator spines 402 and 404 with a substantially more uniform amplitude
along the length of the first and second resonator spines 402 and 404, as described
in greater detail herein. Furthermore, amplitude variations of the clock signal CLK
resulting from additional frequency modes that are stimulated when the operating frequency
differs from the as-fabricated resonant frequency of the respective first and second
resonator spines 402 and 404, and the ribs connected to the first and second resonator
spines 402 and 404, can be suppressed based on the multiple conductive couplings of
the clock signal CLK to the first and second resonator spines 402 and 404, as described
in greater detail herein.
[0025] FIG. 5 illustrates an example diagram 500 of resonator spines. The resonator spines
are demonstrated in the example of FIG. 5 as a first resonator spine 502 and a second
resonator spine 504. The first and second resonator spines 502 and 504 can correspond
to approximately identical resonator spines, as described herein, to demonstrate the
effects of a single coupling of the clock signal CLK to each of the first resonator
spine 502 and the second resonator spine 504. The resonator spines 502 and 504 in
the example of FIG. 5 therefore demonstrate the relative amplitude variation of the
clock signal CLK propagating therein.
[0026] In the example of FIG. 5, the first and second resonator spines 502 and 504 are conductively
coupled by a periodic arrangement of resonator ribs 506. The first resonator spine
502 is demonstrated as receiving the clock signal CLK
A at an approximate midpoint along the length of the first resonator spine 502 and
the resonator spine 504 is demonstrated as receiving the clock signal CLK
B at an approximate midpoint along the length of the second resonator spine 504. Therefore,
the clock signals CLK
A and CLK
B are conductively coupled to the respective first and second resonator spines 502
and 504 at an approximately same location along the length of the respective first
and second resonator spines 502 and 504. As an example, the clock signals CLK
A and CLK
B can be approximately the same, such as described above in the example of FIG. 2.
[0027] In the example of FIG. 5, the variation of the voltage amplitude of the clock signals
CLK
A and CLK
B is plotted along the length of the resonator spines 502 and 504 on a graph 508. Variations
of the frequency of the clock signals CLK
A and CLK
B can result in amplitude variations of the clock signals CLK
A and CLK
B along the length of the resonator spines 502 and 504. The amplitude of the clock
signals CLK
A and CLK
B is demonstrated in the graph 508 as varying relative to an amplitude I
CLK0 that corresponds to a frequency of the clock signals CLK
A and CLK
B that is equal to the resonant frequency of the first and second resonator spines
502 and 504. Therefore, the amplitude of the clock signals CLK
A and CLK
B varies along the length of the resonator spines 502 and 504 based on a variation
in frequency of the clock signals CLK
A and CLK
B relative to the resonant frequency of the resonator spines 502 and 504.
[0028] In the example of FIG. 5, the solid line amplitude in the graph 508 corresponds to
a frequency of the clock signals CLK
A and CLK
B that is greater than the resonant frequency of the resonator spines 502 and 504,
and the dotted line amplitude in the graph 508 corresponds to a frequency of the clock
signals CLK
A and CLK
B that is less than the resonant frequency of the resonator spines 502 and 504 (e.g.,
approximately equal and opposite the resonant frequency relative to the solid line).
As demonstrated in the example of FIG. 5, the amplitude of the clock signals CLK
A and CLK
B, driven above the resonant frequency of the resonator spines 502
and 504, is demonstrated as varying along the length of the resonator spines 502 and
504 from the amplitude I
CLK0 at a location of the conductive coupling of the clock signals CLK
A and CLK
B to the respective first and second resonator spines 502 and 504 to an amplitude I
CLK1 at the distal ends of the first and second resonator spines 502 and 504. Similarly,
the amplitude of the clock signals CLK
A and CLK
B, driven below the resonant frequency of the resonator spines 502 and504, is demonstrated
as varying along the length of the resonator spines 502 and 504 from the amplitude
I
CLK0 at a location of the conductive coupling of the clock signals CLK
A and CLK
B to the respective first and second resonator spines 502 and 504 to an amplitude -I
CLK1 at the distal ends of the first and second resonator spines 502 and 504. Therefore,
at frequencies of the clock signals CLK
A and CLK
B that are greater than or less than the resonant frequency of the resonator spines
502 and 504, the amplitude of the clock signals CLK
A and CLK
B can exhibit errors relative to the amplitude I
CLK0 along the length of the resonator spines 502 and 504 at distances away from the conductive
coupling of the clock signals CLK
A and CLK
B to the respective first and second resonator spines 502 and 504.
[0029] FIG. 6 illustrates another example diagram 600 of resonator spines. The resonator
spines are demonstrated in the example of FIG. 6 as a first resonator spine 602 and
a second resonator spine 604. The first and second resonator spines 602 and 604 can
correspond to approximately identical resonator spines, as described herein, to demonstrate
the effects of multiple couplings of the clock signal CLK to each of the first resonator
spine 602 and the second resonator spine 604. The resonator spines 602 and 604 in
the example of FIG. 6 therefore demonstrate the relative amplitude variation of the
clock signal CLK propagating therein.
[0030] In the example of FIG. 6, the first and second resonator spines 602 and 604 are conductively
coupled by a periodic arrangement of resonator ribs 606. The first resonator spine
602 is demonstrated as receiving a clock signal CLK
A and a clock signal CLK
B at points approximately one quarter of the length of the first resonator spine 602
from the respective ends of the first resonator spine 602. Similarly, the second resonator
spine 604 is demonstrated as receiving a clock signal CLKc and a clock signal CLK
D at points approximately one quarter of the length of the second resonator spine 604
from the respective ends of the second resonator spine 604. Therefore, the clock signals
CLK
A and CLKc are located at approximately the same location along the lengths of the
respective resonator spines 602 and 604, and the clock signals CLK
B and CLK
D are located at approximately the same location along the lengths of the respective
resonator spines 602 and 604.
[0031] In the example of FIG. 6, the variation of the voltage amplitude of the clock signals
CLK
A, CLK
B, CLK
C, and CLK
D is plotted along the length of the resonator spines 602 and 604 on a graph 608. Similar
to as described above in the example of FIG. 5, inherent variations of the frequency
of the clock signals CLK
A, CLK
B, CLK
C, and CLK
D can result in amplitude variations of the clock signals CLK
A, CLK
B, CLK
C, and CLK
D along the length of the resonator spines 602 and 604 relative to the amplitude I
CLK0 (e.g., corresponding to the resonant frequency of the first and second resonator
spines 602 and 604). Therefore, the amplitude of the clock signals CLK
A, CLK
B, CLK
C, and CLK
D varies along the length of the resonator spines 602 and 604 based on a variation
in frequency of the clock signals CLK
A and CLK
B relative to the resonant frequency of the resonator spines 602 and 604.
[0032] In the example of FIG. 6, the solid line amplitude in the graph 608 corresponds to
a frequency of the clock signals CLK
A, CLK
B, CLK
C, and CLK
D that is greater than the resonant frequency of the resonator spines 602 and 604,
and the dotted line amplitude in the graph 608 corresponds to a frequency of the clock
signals CLK
A, CLK
B, CLK
C, and CLK
D that is less than the resonant frequency of the resonator spines 602 and 604 (e.g.,
approximately equal and opposite the resonant frequency relative to the solid line).
As demonstrated in the example of FIG. 6, the amplitude of the clock signals CLK
A, CLK
B, CLKc, and CLK
D, driven above the resonant frequency of the resonator spines 602 and 604, is demonstrated
as varying along the length of the resonator spines 602 and 604 from the amplitude
I
CLK0 at locations of the conductive coupling of the clock signals CLK
A, CLK
B, CLK
C, and CLK
D to the respective first and second resonator spines 602 and 604 to an amplitude I
CLK2 between the conductive couplings of the clock signals CLK
A, CLK
B, CLK
C, and CLK
D to the respective first and second resonator spines 602 and 604 and at the distal
ends of the first and second resonator spines 602 and 604. Similarly, the amplitude
of the clock signals CLK
A, CLK
B, CLK
C, and CLK
D, driven below the resonant frequency of the resonator spines 602 and 604, is demonstrated
as varying along the length of the resonator spines 602 and 604 from the amplitude
I
CLK0 at locations of the conductive coupling of the clock signals CLK
A, CLK
B, CLKc, and CLK
D to the respective first and second resonator spines 602 and 604 to an amplitude -I
CLK2 between the conductive couplings of the clock signals CLK
A, CLK
B, CLK
C, and CLK
D to the respective first and second resonator spines 602 and 604 and at the distal
ends of the first and second resonator spines 602 and 604.
[0033] The amplitude I
CLK2 in the example of FIG. 6 is less than the amplitude I
CLK1 in the example of FIG. 5. Therefore, the diagram 600 demonstrates that multiple conductive
couplings of the clock signal CLK along the length of a resonator spine results in
suppression of amplitude variations of the clock signal CLK resulting from frequency
deviations of the clock signal CLK (e.g., relative to the resonant frequency of the
respective resonator spine). Accordingly, by providing multiple couplings of the clock
signal CLK to a given resonator spine, the amplitude of the clock signal CLK can exhibit
greater uniformity along the length of the respective resonator spine.
[0034] Referring back to the example of FIG. 4, as described above, the first and second
resonator spine 402 and 404 can have an approximately equal length. The example of
FIG. 4 demonstrates that the coupling of the clock signals CLK
A through CLK
F to the first resonator spine 402 is staggered relative to the coupling of the clock
signals CLK
G through CLK
K to the second resonator spine 404. Therefore, the coupling of a set of the resonant
transmission lines 204 to the first resonator spine 402 is offset from the coupling
of a set of the resonant transmission lines 204 to the second resonator spine 404
along the relative lengths of the first and second resonator spines from a first end
of the each of the first and second resonator spines 402 and 404 to a second end of
each of the first and second resonator spines 402 and 404.
[0035] As also described above, at least one of the resonator ribs 408 in a given set of
the resonator ribs 408 can be conductively coupled to both of the first and second
resonator spines 402 and 404. As a result, based on the relative staggered coupling
of the resonant transmission lines 204 to the resonator spines 402 and 404, based
on the coupling of the resonator ribs 408 to both of the resonator spines 402 and
404, and based on the dimensions of the resonator ribs 408 (e.g., approximately equal
in length to a wavelength of the clock signal CLK), the amplitude variations of the
clock signal CLK can be further suppressed. For example, the portions of the resonator
spine 402 between sets of resonator ribs 408 that do not have a conductive coupling
to a resonator 204 can likewise exhibit suppression of the amplitude variation of
the clock signal CLK, similar to portions of the resonator spines 402 and 404 that
have direct conductive coupling to the resonant transmission lines 204. Accordingly,
the amplitude variations of the clock signal CLK can be suppressed on multiple resonator
spines based on fewer conductive couplings to resonant transmission lines of the resonator
feed network, thus reducing circuit complexity and cost.
[0036] As described above, amplitude variations of the clock signal CLK resulting from additional
frequency modes that deviate from the resonant frequency of a resonator spine can
be suppressed based on the multiple conductive couplings of the clock signal CLK to
the resonator spine. FIG. 7 illustrates another example diagram 700 of resonator spines.
The resonator spines are demonstrated in the example of FIG. 7 as a first resonator
spine 702 and a second resonator spine 704. The first and second resonator spines
702 and 704 can correspond to approximately identical resonator spines, as described
herein, to demonstrate the effects of multiple couplings of the clock signal CLK to
each of the first resonator spine 702 and the second resonator spine 704. The resonator
spines 702 and 704 in the example of FIG. 7 therefore demonstrate the relative amplitude
variation of the clock signal CLK propagating therein.
[0037] In the example of FIG. 7, the first and second resonator spines 702 and 704 are conductively
coupled by a periodic arrangement of resonator ribs 706. The first resonator spine
702 is demonstrated as receiving a clock signal CLK
A at a first end of the first resonator spine 702 and a clock signal CLK
B at approximate two-thirds the length of the first resonator spine 702 from the first
end of the first resonator spine 702. Similarly, the second resonator spine 704 is
demonstrated as receiving a clock signal CLKc at approximate one-third the length
of the second resonator spine 704 from the first end of the second resonator spine
704 and a clock signal CLK
D at a second end of the second resonator spine 704 opposite the first end. Therefore,
the clock signals CLK
A, CLK
B, CLK
C, and CLK
D are staggered along the lengths of the respective resonator spines 702 and 704, similar
to as described above in the example of FIG. 4.
[0038] In the example of FIG. 7, the variation of the voltage amplitude of the clock signals
CLK
A, CLK
B, CLK
C, and CLK
D is plotted along the length of the resonator spines 702 and 704 on a graph 708. Similar
to as described above in the example of FIG. 5, inherent variations of the frequency
of the clock signals CLK
A, CLK
B, CLK
C, and CLK
D can result in amplitude variations of the clock signals CLK
A, CLK
B, CLK
C, and CLK
D along the length of the resonator spines 702 and 704 relative to the amplitude I
CLK0 (e.g., corresponding to the resonant frequency of the first and second resonator
spines 702 and 704). Therefore, the amplitude of the clock signals CLK
A, CLK
B, CLK
C, and CLK
D varies along the length of the resonator spines 702 and 704 based on a variation
in frequency of the clock signals CLK
A and CLK
B relative to the resonant frequency of the resonator spines 702 and 704.
[0039] In the example of FIG. 7, the solid line amplitude in the graph 708 corresponds to
a frequency of the clock signals CLK
A, CLK
B, CLK
C, and CLK
D that is greater than the resonant frequency of the resonator spines 702 and 704,
and the dotted line amplitude in the graph 708 corresponds to a frequency of the clock
signals CLK
A, CLK
B, CLK
C, and CLK
D that is less than the resonant frequency of the resonator spines 702 and 704 (e.g.,
approximately equal and opposite the resonant frequency relative to the solid line).
As demonstrated in the example of FIG. 7, the amplitude of the clock signals CLK
A, CLK
B, CLK
C, and CLK
D, driven above the resonant frequency of the resonator spines 702 and 704, is demonstrated
as varying along the length of the resonator spines 702 and 704 from the amplitude
I
CLK0 at locations of any of the conductive coupling of the clock signals CLK
A, CLK
B, CLKc, and CLK
D to the respective one of the first and second resonator spines 702 and 704 to an
amplitude I
CLK3 between any of the conductive couplings of the clock signals CLK
A, CLK
B, CLK
C, and CLK
D to the respective first and second resonator spines 702 and 704. Similarly, the amplitude
of the clock signals CLK
A, CLK
B, CLK
C, and CLK
D, driven below the resonant frequency of the resonator spines 702 and 704, is demonstrated
as varying along the length of the resonator spines 702 and 704 from the amplitude
I
CLK0 at any of the locations of the conductive coupling of the clock signals CLK
A, CLK
B, CLK
C, and CLK
D to the respective first and second resonator spines 702 and 704 to an amplitude -I
CLK3 between any of the conductive couplings of the clock signals CLK
A, CLK
B, CLK
C, and CLK
D to the respective first and second resonator spines 702 and 704.
[0040] The amplitude I
CLK3 in the example of FIG. 7 is less than the amplitude I
CLK2 in the example of FIG. 6. Therefore, the diagram 700 demonstrates that multiple conductive
couplings of the clock signal CLK at staggered locations along the length of multiple
resonator spines relative to each other, with cross-conductive coupling via resonator
ribs, results in further suppression of amplitude variations of the clock signal CLK
resulting from frequency deviations of the clock signal CLK (e.g., relative to the
resonant frequency of the respective resonator spine). Accordingly, by providing multiple
staggered couplings of the clock signal CLK to a multiple resonator spines, with the
staggering being relative to each other on the different resonator spines, the amplitude
of the clock signal CLK can exhibit greater uniformity along the length of the respective
resonator spines. As described above in the example of FIG. 4, by providing fewer
conductive couplings to resonant transmission lines of the resonator feed network,
the complexity and cost of the resonator feed network that provides the clock signal
CLK can be significantly reduced.
[0041] As a result of the amplitude variation suppression described herein, fabrication
process tolerance mismatches that can result in changes to the frequency of the clock
signal CLK and/or the resonant frequency of the respective resonator spine can be
compensated for by coupling the clock signal to multiple locations along the length
of the one or more resonator spines. Accordingly, similar to as described above, resonator
ribs (e.g., the resonator ribs 408 in the example of FIG. 4) can be conductively coupled
at multiple locations along the length of the resonator spine 704 to propagate the
clock signal CLK at approximately uniform amplitudes.
[0042] FIG. 8 illustrates an example diagram 800 of resonator feed networks. The diagram
800 include a first resonator feed network 802 and second resonator feed network 804.
As an example, the resonator feed networks 802 and 804 can be coupled to the substrate
of a carrier supporting multiple ICs (e.g., via bump bonds) to provide the clock signal
CLK to the remaining portions of a given resonator system (e.g., resonator spine(s)
and rib(s) on multiple ICs), as described herein. The resonator feed networks 802
and 804 can correspond to one or more of the resonator feed network(s) 106 in the
example of FIG. 1. Therefore, reference is to be made to the example of FIG. 1 in
the following description of the example of FIG. 8.
[0043] The first resonator feed network 802 includes an oscillator 806 configured to generate
an in-phase portion of the clock signal, demonstrated as an in-phase clock signal
CLK
IP. Similarly, the second resonator feed network 804 includes an oscillator 808 configured
to generate a quadrature-phase portion of the clock signal, demonstrated as a quadrature-phase
clock signal CLK
QP. As an example, the in-phase and quadrature-phase clock signals CLK
IP and CLK
QP can be sinusoidal clock signals. For example, the in-phase and quadrature-phase clock
signals CLK
IP and CLK
QP can be provided in a reciprocal quantum logic (RQL) circuit system.
[0044] In the example of FIG. 8, the first resonator feed network 802 also includes a plurality
of resonant transmission lines 810 and the second resonator feed network 804 includes
a plurality of resonant transmission lines 812. The resonant transmission lines 810
are demonstrated as conductively coupled together and to the oscillator 806 at a node
814 at a first end, and include respective outputs 816 at a second end. Similarly,
the resonant transmission lines 812 are demonstrated as conductively coupled together
and to the oscillator 808 at a node 818 at a first end, and include respective outputs
820 at a second end. In the example of FIG. 8, the outputs 816 and 820 are each demonstrated
as a quantity of seven, and thus provide respective approximately identical clock
signals CLK
A through CLK
G and clock signals CLK
F through CLK
N, respectively. However, other quantities greater than or less than seven for each
of the resonator feed networks 802 and 804 are possible for the clock distribution
system, as described herein. As described herein, the clock signals CLK
A through CLK
G correspond to approximately equal copies of the in-phase clock signal CLK
IP, and the clock signals CLK
H through CLK
N correspond to approximately equal copies of the quadrature-phase clock signal CLK
QP. Therefore, the clock signals CLK
A through CLK
N are all approximately equal with respect to frequency and amplitude, with the clock
signals CLK
H through CLK
N being approximately 90° out-of-phase relative to the clock signals CLK
A through CLK
G.
[0045] Similar to as described above in the example of FIG. 2, the resonant transmission
lines 810 and 812 are each demonstrated as including two transmission line segments
822 that each have a length of λ/4. Therefore, the total length of each of the resonant
transmission lines 810 and 812 is approximately λ/2, and thus approximately half the
wavelength of the clock signal CLK. As a result, the length between any two of the
outputs 816 or between any two of the outputs 820, through a total of four of the
transmission line segments 822, is approximately one wavelength "λ" of the clock signals
CLK
IP and CLK
QP.
[0046] FIG. 9 illustrates another example of a clock distribution system 900. The clock
distribution system 900 can correspond to a portion of the clock distribution system
102 in the example of FIG. 1. Therefore, reference is to be made to the example of
FIGS. 1 and 8 in the following description of the example of FIG. 9.
[0047] The clock distribution system 900 includes a first resonator spine 902, a second
resonator spine 904, a third resonator spine 906, and a fourth resonator spine 908.
The clock distribution system 900 also includes a plurality of sets of resonator ribs
912 that are each coupled to one or more of the resonator spines 902, 904, 906 and
908. The resonator spines 902, 904, 906 and 908 can nominally be fabricated to be
approximately equal in length.
[0048] The first and third resonator spines 902 and 906 receive the in-phase clock signal
CLK
IP, demonstrated as the respective clock signals CLK
A through CLK
G as described above. In the example of FIG. 9, the clock signals CLK
A through CLK
D are provided to the first resonator spine 902 and the clock signals CLK
E through CLK
G are provided to the third resonator spine 906. Similarly, the second and fourth resonator
spines 904 and 908 receive the quadrature-phase clock signal CLK
QP, demonstrated as the respective clock signals CLK
H through CLK
N as described above. The clock signals CLK
H through CLK
J are provided to the second resonator spine 904 and the clock signals CLK
K through CLK
N are provided to the fourth resonator spine 908.
[0049] The clock signals CLK
A through CLK
G can be provided at locations along the length of the resonator spines 902 and 906
and the clock signals CLK
H through CLK
N can be provided at locations along the length of the resonator spines 904 and 908
at predetermined equal intervals between the respective sets of resonator ribs 910.
As an example, the intervals between each of the conductive coupling of the clock
signals CLK
A through CLK
N to the resonator spines 902, 904, 906, and 908 can be approximately equal along the
length of the respective resonator spines 902, 904, 906, and 908.
[0050] As an example, each of the resonator ribs 912 can be selective coupled to one or
more of the resonator spines 902, 904, 906 and 908, such as to propagate the in-phase
clock signal CLK
IP, the quadrature-phase clock signal CLK
QP, or a combination (e.g., varying phase) therebetween. As described above, the clock
distribution system 900 can include circuits (not shown in the example of FIG. 9)
that are coupled (e.g., inductively) to the resonator ribs 912.
[0051] Each of the resonator spines 902, 904, 906, and 908 can therefore suppress amplitude
variations of the respective clock signals CLK
IP and CLK
QP, similar to as described previously. For example, based on the coupling of multiple
copies of the respective clock signals CLK
IP and CLK
QP (e.g., the clock signals CLK
A through CLK
D to the first resonator spine 902, the clock signals CLK
H through CLK
J to the second resonator spine 904, the clock signals CLK
E through CLK
G to the third resonator spine 906, and the clock signals CLK
K through CLK
N to the fourth resonator spine 908), the clock signals CLK
IP and CLK
QP can propagate with a substantially more uniform amplitude along the length of the
resonator spines 902, 904, 906, and 908, as described above. Furthermore, amplitude
variations of the clock signals CLK
IP and CLK
QP resulting from additional frequency modes that deviate from the resonant frequency
of the respective first and second resonator spines 902, 904, 906, and 908 can be
suppressed based on the multiple conductive couplings of the clock signals CLK
IP and CLK
QP to the respective resonator spines 902, 904, 906, and 908, as described above.
[0052] What have been described above are examples of the present invention. It is, of course,
not possible to describe every conceivable combination of components or methodologies
for purposes of describing the present invention, but one of ordinary skill in the
art will recognize that many further combinations and permutations of the present
invention are possible. Accordingly, the present invention is intended to embrace
all such alterations, modifications and variations that fall within the scope of the
appended claims. Additionally, where the disclosure or claims recite "a," "an," "a
first," or "another" element, or the equivalent thereof, it should be interpreted
to include one or more than one such element, neither requiring nor excluding two
or more such elements. As used herein, the term "includes" means includes but not
limited to, and the term "including" means including but not limited to. The term
"based on" means based at least in part on.
[0053] Aspects of the disclosure may also be defined by the following numbered clauses:
Clause 1. A clock distribution system comprising:
a resonator feed network comprising a plurality of resonant transmission lines that
each propagate a clock signal;
at least one resonator spine, each of the at least one resonator spine being conductively
coupled to at least one of the resonant transmission lines, such that each of the
at least one resonator spine propagates the clock signal; and
at least one resonator rib conductively coupled to at least one of the at least one
resonator spine, each of the at least one resonator rib being arranged as a standing
wave resonator to propagate the clock signal.
Clause 2. The system of clause 1, wherein each of the at least one resonator spine
is conductively coupled to a plurality of the resonant transmission lines of the resonator
feed network at each of a plurality of locations separated by at least one interval
along a length of the respective one of the at least one resonator spine.
Clause 3. The system of clause 2, wherein each of the at least one interval is approximately
equal in length.
Clause 4. The system of clause 1, wherein the at least one resonator spine comprises
a plurality of resonator spines, wherein each of the at least one resonator rib is
conductively coupled to a plurality of the plurality of resonator spines.
Clause 5. The system of clause 4, wherein the plurality of resonant transmission lines
comprises a first set of resonant transmission lines and a second set of resonant
transmission lines, each of the first and second sets of resonant transmission lines
having a quantity greater than one, wherein the first set of resonant transmission
lines is coupled to a first resonator spine of the plurality of resonator spines and
the second set of resonant transmission lines is coupled to a second resonator spine
of the plurality of resonator spines, each of the first and second resonator spines
being conductively coupled to a same one of the at least one resonator rib.
Clause 6. The system of clause 5, wherein the first and second resonator spines are
approximately equal in length, wherein the coupling of the first set of resonant transmission
lines to the first resonator spine is offset from the coupling of the second set of
resonant transmission lines to the second resonator spine along relative lengths of
the first and second resonator spines from a first end of the each of the first and
second resonator spines to a second end of each of the first and second resonator
spines.
Clause 7. The system of clause 1, wherein each of the resonant transmission lines
of the resonator feed network are conductively coupled to each other and to a clock
source at a first end of each of the resonant transmission lines and are conductively
coupled to the at least one resonator spine at a second end of the respective resonant
transmission lines.
Clause 8. The system of clause 7, wherein each of the resonant transmission lines
comprises at least one transmission line having a respective length to provide for
a total length of the resonator approximately equal to one-half of a wavelength of
the clock signal, such that a total distance between a first conductive coupling of
a first resonator of the resonant transmission lines to the at least one resonator
spine and a second conductive coupling of a second resonator of the resonant transmission
lines to the at least one resonator spine is separated by approximately one wavelength
of the clock signal through the first and second resonant transmission lines.
Clause 9. The system of clause 1, wherein the resonator feed network comprises:
a first resonator feed network comprising a first plurality of resonant transmission
lines that each propagate an in-phase clock signal; and
a second resonator feed network comprising a second plurality of resonant transmission
lines that each propagate a quadrature-phase clock signal;
wherein the at least one resonator spine comprises:
at least one first resonator spine conductively coupled to the first plurality of
resonant transmission lines, such that each of the at least one first resonator spine
propagates the in-phase clock signal; and
at least one second resonator spine conductively coupled to the second plurality of
resonant transmission lines, such that each of the at least one second resonator spine
propagates the quadrature-phase clock signal.
Clause 10. The system of clause 1, further comprising at least one transformer-coupling
line, each of the at least one transformer-coupling line being conductively coupled
to an associated circuit and having at least one inductive coupling to the at least
one resonator rib to inductively generate a clock current corresponding to the clock
signal via the inductive coupling to provide functions for the associated circuit.
Clause 11. A clock distribution system comprising:
a resonator feed network comprising a plurality of resonant transmission lines that
each propagate a clock signal;
at least one resonator spine, each of the at least one resonator spine being conductively
coupled to at least one of the resonant transmission lines a plurality of the resonant
transmission lines of the resonator feed network at each of a plurality of locations
separated by at least one interval along a length of the respective one of the at
least one resonator spine, such that each of the at least one resonator spine propagates
the clock signal; and
at least one resonator rib conductively coupled to at least one of the at least one
resonator spine, each of the at least one resonator rib being arranged as a standing
wave resonator to propagate the clock signal.
Clause 12. The system of clause 11, wherein the at least one resonator spine comprises
a plurality of resonator spines, wherein each of the at least one resonator rib is
conductively coupled to a plurality of the plurality of resonator spines, wherein
the plurality of resonant transmission lines comprises a first set of resonant transmission
lines and a second set of resonant transmission lines, each of the first and second
sets of resonant transmission lines having a quantity greater than one, wherein the
first set of resonant transmission lines is coupled to a first resonator spine of
the plurality of resonator spines and the second set of resonant transmission lines
is coupled to a second resonator spine of the plurality of resonator spines, each
of the first and second resonator spines being conductively coupled to a same one
of the at least one resonator rib.
Clause 13. The system of clause 12, wherein the first and second resonator spines
are approximately equal in length, wherein the coupling of the first set of resonant
transmission lines to the first resonator spine is offset from the coupling of the
second set of resonant transmission lines to the second resonator spine along relative
lengths of the first and second resonator spines from a first end of the each of the
first and second resonator spines to a second end of each of the first and second
resonator spines.
Clause 14. The system of clause 11, wherein each of the resonant transmission lines
of the resonator feed network are conductively coupled to each other and to a clock
source at a first end of each of the resonant transmission lines and are conductively
coupled to the at least one resonator spine at a second end of the respective resonant
transmission lines, wherein each of the resonant transmission lines comprises at least
one transmission line having a respective length to provide for a total length of
the resonator approximately equal to one-half of a wavelength of the clock signal,
such that a total distance between a first conductive coupling of a first resonator
of the resonant transmission lines to the at least one resonator spine and a second
conductive coupling of a second resonator of the resonant transmission lines to the
at least one resonator spine is separated by approximately one wavelength of the clock
signal through the first and second resonant transmission lines.
Clause 15. The system of clause 11, wherein the resonator feed network comprises:
a first resonator feed network comprising a first plurality of resonant transmission
lines that each propagate an in-phase clock signal; and
a second resonator feed network comprising a second plurality of resonant transmission
lines that each propagate a quadrature-phase clock signal;
wherein the at least one resonator spine comprises:
at least one first resonator spine conductively coupled to the first plurality of
resonant transmission lines, such that each of the at least one first resonator spine
propagates the in-phase clock signal; and
at least one second resonator spine conductively coupled to the second plurality of
resonant transmission lines, such that each of the at least one second resonator spine
propagates the quadrature-phase clock signal.
Clause 16. A clock distribution system comprising:
a resonator feed network comprising a first set of resonant transmission lines and
a second set of resonant transmission lines, each of the first and second sets of
resonant transmission lines having a quantity greater than one and being configured
to propagate a clock signal;
a first resonator spine conductively coupled to the first set of resonant transmission
lines, such that the first resonator spine propagates the clock signal;
a second resonator spine conductively coupled to the second set of resonant transmission
lines, such that the second resonator spine propagates the clock signal; and
at least one resonator rib conductively coupled to each of the first and second resonator
spines, each of the at least one resonator rib being arranged as a standing wave resonator
to propagate the clock signal.
Clause 17. The system of clause 16, wherein the first and second resonator spines
are approximately equal in length, wherein the coupling of the first set of resonant
transmission lines to the first resonator spine is offset from the coupling of the
second set of resonant transmission lines to the second resonator spine along relative
lengths of the first and second resonator spines from a first end of the each of the
first and second resonator spines to a second end of each of the first and second
resonator spines.
Clause 18. The system of clause 16, wherein each of the resonant transmission lines
of the first and second sets of resonant transmission lines are conductively coupled
to each other and to a clock source at a first end of each of the resonant transmission
lines and are conductively coupled to one of the first and second resonator spines
at a second end of the respective resonant transmission lines.
Clause 19. The system of clause 18, wherein each of the resonant transmission lines
of the first and second sets of resonant transmission lines comprises at least one
transmission line having a respective length to provide for a total length of the
resonator approximately equal to one-half of a wavelength of the clock signal, such
that a total distance between a first conductive coupling of a first resonator of
the resonant transmission lines to one of the first and second resonator spines and
a second conductive coupling of a second resonator of the resonant transmission lines
to one of the first and second resonator spines is separated by approximately one
wavelength of the clock signal through the first and second resonant transmission
lines.
Clause 20. The system of clause 16, further comprising at least one transformer-coupling
line, each of the at least one transformer-coupling line being conductively coupled
to an associated circuit and having at least one inductive coupling to the at least
one resonator rib to inductively generate a clock current corresponding to the clock
signal via the inductive coupling to provide functions for the associated circuit.
1. A clock distribution system comprising:
a resonator feed network comprising a plurality of resonant transmission lines that
each propagate a clock signal;
at least one resonator spine, each of the at least one resonator spine being conductively
coupled to at least one of the resonant transmission lines, such that each of the
at least one resonator spine propagates the clock signal; and
at least one resonator rib conductively coupled to at least one of the at least one
resonator spine, each of the at least one resonator rib being arranged as a standing
wave resonator to propagate the clock signal.
2. The system of claim 1, wherein each of the at least one resonator spine is conductively
coupled to a plurality of the resonant transmission lines of the resonator feed network
at each of a plurality of locations separated by at least one interval along a length
of the respective one of the at least one resonator spine.
3. The system of claim 2, wherein each of the at least one interval is approximately
equal in length.
4. The system of claim 1, wherein the at least one resonator spine comprises a plurality
of resonator spines, wherein each of the at least one resonator rib is conductively
coupled to a plurality of the plurality of resonator spines.
5. The system of claim 4, wherein the plurality of resonant transmission lines comprises
a first set of resonant transmission lines and a second set of resonant transmission
lines, each of the first and second sets of resonant transmission lines having a quantity
greater than one, wherein the first set of resonant transmission lines is coupled
to a first resonator spine of the plurality of resonator spines and the second set
of resonant transmission lines is coupled to a second resonator spine of the plurality
of resonator spines, each of the first and second resonator spines being conductively
coupled to a same one of the at least one resonator rib.
6. The system of claim 5, wherein the first and second resonator spines are approximately
equal in length, wherein the coupling of the first set of resonant transmission lines
to the first resonator spine is offset from the coupling of the second set of resonant
transmission lines to the second resonator spine along relative lengths of the first
and second resonator spines from a first end of the each of the first and second resonator
spines to a second end of each of the first and second resonator spines.
7. The system of claim 1, wherein each of the resonant transmission lines of the resonator
feed network are conductively coupled to each other and to a clock source at a first
end of each of the resonant transmission lines and are conductively coupled to the
at least one resonator spine at a second end of the respective resonant transmission
lines.
8. The system of claim 7, wherein each of the resonant transmission lines comprises at
least one transmission line having a respective length to provide for a total length
of the resonator approximately equal to one-half of a wavelength of the clock signal,
such that a total distance between a first conductive coupling of a first resonator
of the resonant transmission lines to the at least one resonator spine and a second
conductive coupling of a second resonator of the resonant transmission lines to the
at least one resonator spine is separated by approximately one wavelength of the clock
signal through the first and second resonant transmission lines.
9. The system of claim 1, wherein the resonator feed network comprises:
a first resonator feed network comprising a first plurality of resonant transmission
lines that each propagate an in-phase clock signal; and
a second resonator feed network comprising a second plurality of resonant transmission
lines that each propagate a quadrature-phase clock signal;
wherein the at least one resonator spine comprises:
at least one first resonator spine conductively coupled to the first plurality of
resonant transmission lines, such that each of the at least one first resonator spine
propagates the in-phase clock signal; and
at least one second resonator spine conductively coupled to the second plurality of
resonant transmission lines, such that each of the at least one second resonator spine
propagates the quadrature-phase clock signal.
10. The system of claim 1, further comprising at least one transformer-coupling line,
each of the at least one transformer-coupling line being conductively coupled to an
associated circuit and having at least one inductive coupling to the at least one
resonator rib to inductively generate a clock current corresponding to the clock signal
via the inductive coupling to provide functions for the associated circuit.
11. A clock distribution system comprising:
a resonator feed network comprising a plurality of resonant transmission lines that
each propagate a clock signal;
at least one resonator spine, each of the at least one resonator spine being conductively
coupled to at least one of the resonant transmission lines a plurality of the resonant
transmission lines of the resonator feed network at each of a plurality of locations
separated by at least one interval along a length of the respective one of the at
least one resonator spine, such that each of the at least one resonator spine propagates
the clock signal; and
at least one resonator rib conductively coupled to at least one of the at least one
resonator spine, each of the at least one resonator rib being arranged as a standing
wave resonator to propagate the clock signal.
12. The system of claim 11, wherein the at least one resonator spine comprises a plurality
of resonator spines, wherein each of the at least one resonator rib is conductively
coupled to a plurality of the plurality of resonator spines, wherein the plurality
of resonant transmission lines comprises a first set of resonant transmission lines
and a second set of resonant transmission lines, each of the first and second sets
of resonant transmission lines having a quantity greater than one, wherein the first
set of resonant transmission lines is coupled to a first resonator spine of the plurality
of resonator spines and the second set of resonant transmission lines is coupled to
a second resonator spine of the plurality of resonator spines, each of the first and
second resonator spines being conductively coupled to a same one of the at least one
resonator rib.
13. The system of claim 12, wherein the first and second resonator spines are approximately
equal in length, wherein the coupling of the first set of resonant transmission lines
to the first resonator spine is offset from the coupling of the second set of resonant
transmission lines to the second resonator spine along relative lengths of the first
and second resonator spines from a first end of the each of the first and second resonator
spines to a second end of each of the first and second resonator spines.
14. The system of claim 11, wherein each of the resonant transmission lines of the resonator
feed network are conductively coupled to each other and to a clock source at a first
end of each of the resonant transmission lines and are conductively coupled to the
at least one resonator spine at a second end of the respective resonant transmission
lines, wherein each of the resonant transmission lines comprises at least one transmission
line having a respective length to provide for a total length of the resonator approximately
equal to one-half of a wavelength of the clock signal, such that a total distance
between a first conductive coupling of a first resonator of the resonant transmission
lines to the at least one resonator spine and a second conductive coupling of a second
resonator of the resonant transmission lines to the at least one resonator spine is
separated by approximately one wavelength of the clock signal through the first and
second resonant transmission lines.
15. The system of claim 11, wherein the resonator feed network comprises:
a first resonator feed network comprising a first plurality of resonant transmission
lines that each propagate an in-phase clock signal; and
a second resonator feed network comprising a second plurality of resonant transmission
lines that each propagate a quadrature-phase clock signal;
wherein the at least one resonator spine comprises:
at least one first resonator spine conductively coupled to the first plurality of
resonant transmission lines, such that each of the at least one first resonator spine
propagates the in-phase clock signal; and
at least one second resonator spine conductively coupled to the second plurality of
resonant transmission lines, such that each of the at least one second resonator spine
propagates the quadrature-phase clock signal.